\begin{table}%t3
\caption{\label{table3}Summary of the properties of the new members of the E+S~systems.}
\small%\centerline
 {
\begin{tabular}{lccccccccccc}
\hline\hline
&&&&&&&&&&& \\[-8pt]
 ID & $\alpha$ & $\delta$ & $v_{\rm rad}$ & $R^a$ & $D^b$ & $m_R$ & $(V-R)$ & $n$ & $r_{\rm e}$ & $\mu_0$ & $\mu_{\rm e}$ \\
    & & & [km s$^{-1}$] & & [Mpc] & [mag] & [mag] & & [kpc] & \multicolumn{2}{c}{ [mag arcsec$^{-2}$]}\\
\hline
RR143\_09192 & 06 47 53.25 & --64 10 55.1 & $3296\pm46~$ & ~3.34 & 0.122 & 17.25 & 0.56 & 1.05 & 1.30 & 21.30 & 23.23 \\
RR143\_24246 & 06 47 07.47 & --64 29 15.8 & $3724\pm73~$ & ~3.87 & 0.269 & 16.95 & 0.34 & 1.57  &  1.40  &  19.73  &  22.80  \\
  & & & & & & & & & & & \\
RR210\_11372 & 12 07 43.28 & --29 43 10.9 & $1927\pm183$ & ~3.08 & 0.117 & 17.59 & 0.50 & 0.83 & 0.97 & 22.24 & 23.68 \\
RR210\_13493$^c$ & 12 06 50.26 & --29 36 23.5 & $2008\pm45~$ & ~9.08 & 0.080 & 14.26 & 0.52 & 1.98 & 1.30 & 18.03 & 21.97 \\
  & & & & & & & & & & & \\
RR216\_03519 & 12 25 17.80 & --39 33 45.6 & $3716\pm134$ & ~2.13 & 0.165 & 17.26 & 0.51 & 1.02 & 1.22 & 21.41 & 23.28 \\
RR216\_04052$^d$ & 12 26 11.30 & --39 34 47.1 & $3193\pm50~$ & ~9.63 & 0.209 & 14.57 & 0.60 & 1.07 & 2.52 & 20.18 & 22.15 \\
RR216\_12209 & 12 25 37.04 & --39 44 36.4 & $2697\pm62~$ & ~5.32 & 0.054 & 15.58 & 0.59 & 0.74 & 2.17 & 21.57 & 22.82 \\
  & & & & & & & & & & & \\
RR242\_08064 & 13 22 10.44 & --43 32 55.6 & $3441\pm60~$ & ~2.58 & 0.202 & 17.85 & 0.64 & 1.21 & 1.32 & 21.88 & 24.15 \\
RR242\_13326 & 13 21 03.88 & --43 36 58.1 & $3172\pm45~$ & ~3.42 & 0.080 & 16.15 & 0.60 & 1.42 & 2.11 & 20.15 & 22.87 \\
RR242\_15689 & 13 21 16.54 & --43 38 53.2 & $3731\pm81~$ & ~7.20 & 0.050 & 17.73 & 0.74 & 1.38 & 0.73 & 20.47 & 23.11 \\
RR242\_20075 & 13 20 26.71 & --43 42 27.5 & $3045\pm52~$ & ~6.63 & 0.120 & 16.33 & 0.55 & 1.51& 1.38 & 20.02 & 22.95 \\
RR242\_22327$^e$ & 13 20 55.54 & --43 44 20.2 & $3237\pm70~$ & ~9.63 & 0.054 & 15.06 & 0.69 & 1.34 & 0.98 & 18.38 & 20.94 \\
RR242\_23187 & 13 21 33.01 & --43 39 43.0 & $3400\pm88~$ & ~0.00 & 0.058 & 17.37 & 0.44 & 0.75 & 0.95 & 20.54 & 21.82 \\
RR242\_24352$^f$ & 13 21 14.82 & --43 45 43.2 & $2697\pm45~$ & 10.05 & 0.050 & 13.71 & 0.62 & 2.35 & 1.68 & 16.00 & 20.76 \\
RR242\_25575 & 13 19 44.25 & --43 46 28.0 & $2655\pm84~$ & ~4.26 & 0.239 & 16.42 & 0.60 & 2.24 & 1.73 & 19.02 & 23.53 \\
RR242\_28727 & 13 21 22.55 & --43 43 21.6 & $3017\pm87~$ & ~6.80 & 0.030 & 17.05 & 0.64 & 1.16 & 0.69 & 20.08 & 22.25 \\
RR242\_36267 & 13 20 21.80 & --43 55 38.4 & $2997\pm40~$ & ~3.19 & 0.245 & 18.67 & 0.50 & 0.89 & 1.07 & 22.32 & 23.90 \\
\hline
\end{tabular}}
\medskip
$^a$ Confidence parameter $R$ from the cross-correlation procedure. If $R = 0$ then the lines were measured by hand with {\tt splot};
$^b$~projected distance from the E~member of the pair;
$^c$~RR210\_13493~= 2MASX~J12065029-2936236;
$^d$~RR216\_04052~= 2MASX~J12261133-3934474;
$^e$~RR242\_22327~= ESO~270-~G~001;
$^f$~RR242\_24352~= ESO~270-~G~003.
\end{table}